Research/Sitter/MAGNDATA / 0.735_LaBaMn2O5.mcif

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Spin lattice of LaBaMn2O5Spin lattice of LaBaMn2O5

LaBaMn2O5

MAGNDATA entry 0.735 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 100 K (−173 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 4/n m′ m′ BNS 129.417
Point group4/mm′m′
Parent space groupP 4/n m m No. 129
Spinscollinear · net moment 1 μB per cell
Propagation[0 0 0] 1k
Cella 5.6386 · b 5.6386 · c 7.7799 Å · α 90° · β 90° · γ 90°
Transition100 K (−173 °C)
Measured at1.5 K
Magnetic ionsMn
Largest moment component3.2 μB
MethodNPD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P 4/n m′ m′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La0.750.250.5
Ba1Ba0.750.250
Mn1Mn0.250.250.263700−2.72.7
Mn2Mn0.250.250.7511003.23.2
O1O0.49080.49080.2999
O2O0.250.250.0061

Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

F. Millange et al. Chem. Mater. (1998) · doi:10.1021/cm980130v

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.735_LaBaMn2O5.mcif from MAGNDATA · entry page

sha256 of this copy: 981122e931016b8045221cbe760cc8fa95af780a9f58a00484e416d98879f7e0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.735_LaBaMn2O5.mcif.